The relativistic kinetic energy is given by
"E_{kinetic} = \\frac{mc^2}{\\sqrt{1-\\frac{v^2}{c^2}}} - mc^2"
We see that it is a growing function of "v^2" , is 0 for "v=0" and goes to "+\\infty" when "v" approaches "c" . We can even show that for "v \\ll c" we have the classical expression of kinetic energy:
"E \\underset{v\/c\\to 0}{\\sim} mc^2 (1+\\frac{1}{2}\\frac{v^2}{c^2}) - mc^2 = \\frac{mv^2}{2}"
The relativistic kinetic energy have the same physical meaning: it is the energy of an object related to it's movement independently of a direction.
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